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VUV Spectroscopy of Atoms, Molecules and Surfaces

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148<br />

The following three chapters are devoted to the spectroscopy <strong>of</strong> negative<br />

ions which are particularly interesting from an astrophysical- <strong>and</strong> a theoretical<br />

point <strong>of</strong> view. The structure, or energy-level diagram, <strong>of</strong> a negative ion is<br />

markedly different from that <strong>of</strong> a neutral atom or -molecule due to the correlation<br />

effects introduced by the presence <strong>of</strong> the extra electron. In general,<br />

only a single bound state exists but the single-electron continuum may reveal<br />

a rich structure <strong>of</strong> doubly-excited states, resonances, that are <strong>of</strong>ten associated<br />

with excited states <strong>of</strong> the corresponding neutral atom or -molecule. A<br />

doubly-excited state typically decays by electron emission in a process known<br />

as autodetachment, leaving the resulting neutral system in its ground state or<br />

a lower-lying excited state. In chapter 2 a general introduction to the properties<br />

<strong>of</strong> negative ions is given, including an overview <strong>of</strong> the present knowledge<br />

obtained from spectroscopic studies <strong>and</strong> the theoretical approaches currently<br />

applied to model their structure.<br />

An experimental technique for Doppler-tuned <strong>VUV</strong> spectroscopy <strong>of</strong> highlying<br />

doubly-excited states <strong>of</strong> the fundamental negative-ion system H− ,has<br />

previously been implemented at the storage ring ASTRID. In these studies<br />

use was made <strong>of</strong> a fixed-frequency <strong>VUV</strong> light source based on the non-linear<br />

frequency-upconversion <strong>of</strong> visible laser light by a process known as harmonic<br />

generation. The unprecedented spectral resolution achieved with this technique<br />

has allowed the observation <strong>of</strong> previously un-resolved resonances <strong>and</strong><br />

has recently been improved by the application <strong>of</strong> the electron cooler <strong>of</strong> the<br />

storage ring. This has allowed the first precise measurement <strong>of</strong> the spectral<br />

width <strong>of</strong> one <strong>of</strong> these resonances, providing the first critical test <strong>of</strong> a number<br />

<strong>of</strong> theoretical models as described in chapter 3.<br />

The ASTRID storage ring has also previously been successfully used for<br />

lifetime measurements <strong>of</strong> metastable, doubly-excited, autodetaching states <strong>of</strong><br />

atomic negative ions with lifetimes in the µs–ms range. The spectral widths<br />

<strong>of</strong> such states are too narrow that they can be resolved by ordinary laserspectroscopic<br />

methods. In the storage ring the ions are allowed to circulate<br />

for several lifetimes, facilitating a precise measurement <strong>of</strong> the decay rate as a<br />

function <strong>of</strong> time. In the experiments described in chapter 4this method has<br />

been applied to lifetime measurements on unknown metastable states <strong>of</strong> N − 2<br />

<strong>and</strong> CO − 2<br />

which do not exist as stable ground-state ions. By a co-operation<br />

with theorists, the lifetimes observed have been assigned to a previously unexplored<br />

class <strong>of</strong> high-spin negative-ion states.<br />

The focus <strong>of</strong> chapter 5 is on the construction <strong>of</strong> an experimental setup aiming<br />

at studies <strong>of</strong> structural dynamical processes at surfaces with a femtosecond<br />

time resolution. Emphasis is given to chemical reactions <strong>of</strong> gas-phase<br />

molecules which are enhanced, or catalyzed, by the presence <strong>of</strong> the surface,<br />

in particular to the desorption step, by which the product molecules escape

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